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CEC Abstracts in PDF format (as of 7/3/07) - CEC-ICMC 2013

CEC Abstracts in PDF format (as of 7/3/07) - CEC-ICMC 2013

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<strong>CEC</strong> 20<strong>07</strong> - <strong>Abstracts</strong><br />

C1-F-02 Cryogenic Thermal Performance Test<strong>in</strong>g <strong>of</strong><br />

Bulk-Fill and Aerogel Insulation Materials<br />

B.E. Scholtens, J.E. Fesmire, J.P. S<strong>as</strong>s, NASA KSC;<br />

S.D. Augustynowicz, K.W. Heckle, Sierra Lobo, Inc.<br />

The research test<strong>in</strong>g and demonstration <strong>of</strong> new bulk-fill materials for<br />

cryogenic thermal <strong>in</strong>sulation systems w<strong>as</strong> performed by the<br />

Cryogenics Test Laboratory at NASA Kennedy Space Center.<br />

Thermal conductivity test<strong>in</strong>g under actual-use cryogenic conditions is<br />

a key to understand<strong>in</strong>g the total system performance encomp<strong>as</strong>s<strong>in</strong>g<br />

eng<strong>in</strong>eer<strong>in</strong>g, economics, and materials factors. A number <strong>of</strong> bulk fill<br />

<strong>in</strong>sulation materials, <strong>in</strong>clud<strong>in</strong>g aerogel beads, gl<strong>as</strong>s bubbles, and<br />

perlite powder, were tested us<strong>in</strong>g a new cyl<strong>in</strong>drical cryostat. Boundary<br />

temperatures for the liquid nitrogen boil-<strong>of</strong>f method were typically<br />

293 K and 77 K. Tests were performed <strong>as</strong> a function <strong>of</strong> vacuum<br />

pressure level from high vacuum to no vacuum conditions. Results<br />

are compared with other complementary test methods <strong>in</strong> the range <strong>of</strong><br />

300 K to 10 K. Various test<strong>in</strong>g techniques are shown to be required to<br />

obta<strong>in</strong> a complete understand<strong>in</strong>g <strong>of</strong> the operat<strong>in</strong>g performance <strong>of</strong> a<br />

material and to establish a b<strong>as</strong>is for answers to design eng<strong>in</strong>eer<strong>in</strong>g<br />

questions.<br />

C1-F-03 Multilauer Insulation for Atl<strong>as</strong><br />

S. Kozub, K. Polkovnikov, A. Hartchenko, Institute for<br />

High Energy Physics.<br />

Multilayer <strong>in</strong>sulation consists <strong>of</strong> alum<strong>in</strong>ized mylar and mylar cloth<br />

spacer for ATLAS (LHC) w<strong>as</strong> manufactured and tested at Institute for<br />

High Energy Physics (Protv<strong>in</strong>o, Russia). The paper presents<br />

description <strong>of</strong> facility for the multilayer <strong>in</strong>sulation test <strong>as</strong> well <strong>as</strong><br />

results <strong>of</strong> g<strong>as</strong>s<strong>in</strong>g <strong>in</strong> vacuum rate and heat leakage me<strong>as</strong>urements for<br />

the <strong>in</strong>sulation.<br />

C1-F-04 Test<strong>in</strong>g <strong>of</strong> a Vacuum Insulated Flexible L<strong>in</strong>e<br />

With Flow<strong>in</strong>g Liquid Nitrogen Dur<strong>in</strong>g the Loss <strong>of</strong><br />

Insulat<strong>in</strong>g Vacuum<br />

J.A. Demko, M.J. Gouge, R.C. Duckworth, Oak<br />

Ridge National Laboratory; M. Roden, Southwire<br />

Co..<br />

Long length vacuum <strong>in</strong>sulated l<strong>in</strong>es are used to carry flow<strong>in</strong>g liquid<br />

nitrogen <strong>in</strong> several high temperature superconduct<strong>in</strong>g cable projects.<br />

An important, but rare, failure scenario is the abrupt or cat<strong>as</strong>trophic<br />

loss <strong>of</strong> the thermal <strong>in</strong>sulat<strong>in</strong>g vacuum produc<strong>in</strong>g a rapid <strong>in</strong>cre<strong>as</strong>e <strong>in</strong><br />

heat transfer to the liquid nitrogen stream. In this <strong>in</strong>vestigation, a<br />

vacuum super<strong>in</strong>sulated 3 <strong>in</strong>ch by 5 <strong>in</strong>ch NPS is subjected to an abrupt<br />

loss <strong>of</strong> vacuum <strong>in</strong> order to me<strong>as</strong>ure the response <strong>of</strong> a flow<strong>in</strong>g liquid<br />

nitrogen stream and the temperature response <strong>of</strong> the cryostat. The<br />

me<strong>as</strong>ured outlet stream temperature h<strong>as</strong> a slight peak shortly after the<br />

loss <strong>of</strong> vacuum <strong>in</strong>cident and drops to a steady state value. The heat<br />

loads me<strong>as</strong>ured before and after the vacuum loss event are reported.<br />

Some me<strong>as</strong>urements <strong>of</strong> the temperatures <strong>in</strong> the multi-layer<br />

super<strong>in</strong>sulation are also discussed.<br />

Research sponsored by the U.S. Department <strong>of</strong> Energy - Office <strong>of</strong><br />

Electricity Delivery and Energy Reliability, Superconductivity<br />

Program for Electric Power Systems under contract DE-AC05-<br />

00OR22725 with Oak Ridge National Laboratory, managed and<br />

operated by UT-Battelle, LLC.<br />

C1-F-05 Radiation heat me<strong>as</strong>urement on thermally<br />

isolated double-pipe for DC superconduct<strong>in</strong>g power<br />

transmission<br />

M. Hamabe, S. Yamaguchi, Chubu University; A.<br />

N<strong>in</strong>omiya, Seikei University; Y. Ishiguro, S. Kusaka,<br />

JFE Steel Corporation.<br />

Multilayer <strong>in</strong>sulation (MLI) is a strong tool to reduce the radiation<br />

heat and is widely used for the cryogenic systems. However, the use<br />

<strong>of</strong> the MLI leads to a huge <strong>in</strong>cre<strong>as</strong>e <strong>of</strong> the surface area <strong>in</strong> vacuum; it<br />

takes extremely long time to reach a satisfactory vacuum for the<br />

thermal isolation, or the nitrogen g<strong>as</strong> flush<strong>in</strong>g is needed several times.<br />

We have started the experiment by us<strong>in</strong>g the test bench <strong>of</strong> the DC<br />

superconduct<strong>in</strong>g (DC-SC) power cable <strong>in</strong> Chubu University. S<strong>in</strong>ce the<br />

DC-SC power cable is free from the AC losses, the acceptable<br />

radiation heat can be higher for this cable than the AC-SC power<br />

cable. Therefore, we are study<strong>in</strong>g the possibility <strong>of</strong> the radiation shield<br />

without the MLI. The vacuum pump<strong>in</strong>g process and the radiation heat<br />

are me<strong>as</strong>ured for the thermally isolated double-pipes (<strong>of</strong> the same size<br />

<strong>as</strong> those for the DC-SC PT cable) with the various surfaces. While the<br />

radiation heat for the liquid-nitrogen-filled double-pipe with the MLI<br />

radiation shield w<strong>as</strong> 1/100 <strong>of</strong> that with the bare sta<strong>in</strong>less steel surface,<br />

the reachable vacuum pressure with the MLI w<strong>as</strong> 10 times poorer than<br />

that with the bare surface. We will also discuss a novel and<br />

convenient radiation shield<strong>in</strong>g method for the different surface<br />

processes <strong>in</strong> this work.<br />

C1-F-06 Low temperature heat transfer properties <strong>of</strong><br />

electrical <strong>in</strong>sulation for the Next European Dipole<br />

J. Pol<strong>in</strong>ski, B. Baudouy, CEA Saclay; S. Canfer, G.<br />

Ellwood, RAL.<br />

The heat transfer properties <strong>of</strong> the electrical multilayer <strong>in</strong>sulations <strong>of</strong><br />

the Next European dipole h<strong>as</strong> been tested under various conditions at<br />

low temperature. The electrical <strong>in</strong>sulation is made <strong>of</strong> E-gl<strong>as</strong>s fibre<br />

with a pla<strong>in</strong> weave and RAL epoxy system 227 (DGEBF epoxy res<strong>in</strong><br />

and DETD aromatic hardener). The samples have been tested <strong>in</strong><br />

superfluid helium where heat is applied perpendicularly to the fibres<br />

between 1.6 K to 2.1 K and their thermal conductivity, longitud<strong>in</strong>al to<br />

the fibres, had been also me<strong>as</strong>ured at low temperature below 77 K.<br />

This work w<strong>as</strong> supported <strong>in</strong> part by the European Community–<br />

Research Infr<strong>as</strong>tructure Activity under the FP6 “Structur<strong>in</strong>g the<br />

European Research Area” program (CARE, contract number RII3-<br />

CT-2003-506395).<br />

C1-F-<strong>07</strong> Flexible Aerogel Composites for Cryogenic<br />

Insulation<br />

R. Trifu, R. Begag, G. Gould, O. Evans, S. White,<br />

Aspen Aerogels, Inc..<br />

Low-density, flexible aerogel composites <strong>of</strong>fer a variety <strong>of</strong><br />

performance advantages over other <strong>in</strong>sulation materials for cryogenic<br />

<strong>in</strong>sulation applications, particularly Multi-Layer Insulation (MLI).<br />

These advantages <strong>in</strong>clude reduced weight, <strong>in</strong>cre<strong>as</strong>ed durability, lower<br />

total costs, and dramatic improvements <strong>in</strong> lead-times required for<br />

fabrication / <strong>in</strong>stallation <strong>of</strong> the <strong>in</strong>sulation with equal thermal<br />

performance. Additionally, large error bars <strong>of</strong>ten <strong>as</strong>sociated with the<br />

thermal model<strong>in</strong>g <strong>of</strong> MLI can be elim<strong>in</strong>ated with the use <strong>of</strong> aerogel<br />

composites. These low density aerogel composites have been found<br />

to be compatible with sensitive space sensors. Outg<strong>as</strong>s<strong>in</strong>g data along<br />

with encapsulation concepts for the aerogel composites will be<br />

discussed. A ‘higher’ density aerogel composite for <strong>in</strong>sulat<strong>in</strong>g liquid<br />

oxygen transfer l<strong>in</strong>es and storage conta<strong>in</strong>ers will also be presented.<br />

Page 6 <strong>of</strong> 53

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